M. Knoop, I. Marzoli, G. Morigi's Ion traps for tomorrow's applications PDF

By M. Knoop, I. Marzoli, G. Morigi

ISBN-10: 1271271281

ISBN-13: 9781271271283

ISBN-10: 1614995257

ISBN-13: 9781614995258

ISBN-10: 1614995265

ISBN-13: 9781614995265

ISBN-10: 8874380933

ISBN-13: 9788874380930

Ion trapping was once first comprehensive in Europe greater than 50 years in the past. because then, study and improvement have elevated gradually, and the final many years have noticeable a striking development in functions, in general because of the development of laser-based concepts for spectroscopy, cooling and the manipulation of ions. these days ion trapping performs a very important position in quite a lot of disciplines, together with atomic and plasma physics, chemistry, excessive precision dimension, excessive power physics and the rising box of quantum applied sciences. This ebook offers lectures and studies from the Enrico Fermi college Ion Traps for Tomorrow's purposes , held in Varenna, Italy, in July 2013. Reflecting the purpose of the college to use range and stimulate pass fertilization, the chosen subject matters and highlights during this publication in part overview the wide variety of topics mentioned through the direction, whereas delivering an outline of this topical area. in addition to offering an invaluable reference consultant, the booklet might be a resource of notion for all these making plans to paintings on ion trapping sooner or later

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Therefore they are often called quasi-stationary states. Next we will find the lowest-order corrections to the static-potential oscillator picture in close analogy to the classical pseudopotential solution presented in the previous section. We also discuss the analogous operator to the number operator for the static-potential harmonic oscillator. 14 D. Leibfried and D. Lucas We first derive an approximate expression for the special solution u(t). Again |ax |, 1 and C±4 = 0 is assumed. Together with the initial conditions of eq.

On the other hand, if no photons are scattered, the ion was projected into state |e by the interaction with the driving field. Depending on the background light scattered into the PMT and its dark count rate, |g and |e can be distinguished with high confidence in rather short detection periods (typically on the order of few 100 μs). Apart from this convenient way of measuring the quantum state, Dehmelt’s proposal triggered a number of theoretical papers on “quantum jumps” between |g and |e that would manifest themselves by extended periods of time with few or many photons detected, respectively, if both transitions are driven simultaneously.

029). 115 + Peik et al. 7(3) corresponding to 58% ground state occupation. The cooling transition was the weakly allowed 5s2 1 S0 → 5s5p 3 P1 intercombination line with an experimentally observed linewidth of Γ = (2π)650 kHz. The trap frequency ν was about (2π)1 MHz. At the University of Innsbruck, ground state cooling was achieved on a single 40 Ca+ ion for various motional frequencies from ν = (2π) 2 MHz . . 4 MHz [108]. The method used was very similar to the experiment in 198 Hg+ . The cooling transition was the well 34 D.

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Ion traps for tomorrow's applications by M. Knoop, I. Marzoli, G. Morigi

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